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QNEET-2013-Ph-1507: NEET 2013 Physics - Class 12 NEET-2013-Ph-1507 Solution: Two pith balls carrying equal charges are suspended from a…

Two pith balls carrying equal charges are suspended from a common point by strings of equal length. The equilibrium separation between them is rr. Now the strings are rigidly clamped at half the height. The equilibrium separation between the balls now becomes:

Multiple Choice Options

  • A - **(A)** 2r3\frac{2r}{\sqrt{3}}
  • B - **(B)** \frac{2r}{3}}
  • C - **(C)** r23\frac{r}{\sqrt[3]{2}}
  • D - **(D)** r2\frac{r}{2}

Step-by-Step Verified Solution

1. Set up the Equilibrium Conditions for Case 1: Let the vertical distance from the suspension point to the line joining the balls be yy, the string length be ll, and the angle with the vertical be θ\theta. Three forces act on each pith ball: � Tension (TT) along the string � Weight (mgmg) pointing straight down � Electrostatic Repulsive Force (FF) acting horizontally: F=q24πε0r2F=\frac{q^{2}}{4\pi \varepsilon _{0}r^{2}} Resolving components at equilibrium: Tcos⁡θ=mgT\cos \theta =mg Tsin⁡θ=FT\sin \theta =F Dividing the two equations gives: tan⁡θ=Fmg\tan \theta =\frac{F}{mg} 2. Apply the Small-Angle Approximation: For small values of θ\theta, we can approximate tan⁡θ≈OppositeAdjacent=r/2y\tan\theta \approx \frac{\text{Opposite}}{\text{Adjacent}} = \frac{r/2}{y}: r2y=q24πε0r2mg  ⟹  y=(2πε0mgq2)r3\frac{r}{2y}=\frac{q^{2}}{4\pi \varepsilon _{0}r^{2}mg}\implies y=\left(\frac{2\pi \varepsilon _{0}mg}{q^{2}}\right)r^{3} This establishes a clean mathematical proportionality: y∝r3orr∝y1/3y\propto r^{3}\quad \text{or}\quad r\propto y^{1/3} 3. Analyze Case 2 (Clamped at half the height): When the strings are fixed at half their original vertical suspension height, the new height becomes y′=y2y' = \frac{y}{2}. Letting the new separation be r′r^{\prime }: y′y=(r′r)3\frac{y^{\prime }}{y}=\left(\frac{r^{\prime }}{r}\right)^{3} Substitute y′=y2y' = \frac{y}{2}: y/2y=(r′r)3  ⟹  12=(r′r)3\frac{y/2}{y}=\left(\frac{r^{\prime }}{r}\right)^{3}\implies \frac{1}{2}=\left(\frac{r^{\prime }}{r}\right)^{3} Taking the cube root of both sides gives the final value: r′r=123  ⟹  r′=r23\frac{r^{\prime }}{r}=\frac{1}{\sqrt[3]{2}}\implies r^{\prime }=\frac{r}{\sqrt[3]{2}}

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